Influence of hydrogen bridges on the magnetic properties of copper(II) bis(trifluoroacetate) complexes

Citation
V. Calvo et al., Influence of hydrogen bridges on the magnetic properties of copper(II) bis(trifluoroacetate) complexes, BOL SOC CH, 45(2), 2000, pp. 259-268
Citations number
24
Categorie Soggetti
Chemistry
Journal title
BOLETIN DE LA SOCIEDAD CHILENA DE QUIMICA
ISSN journal
03661644 → ACNP
Volume
45
Issue
2
Year of publication
2000
Pages
259 - 268
Database
ISI
SICI code
0366-1644(200006)45:2<259:IOHBOT>2.0.ZU;2-O
Abstract
Copper(ll) trifluoroacetate with three coordinated water molecules and two dioxane molecules (1) crystallized as a linear chain surrounded by a net of hydrogen bonds to the dioxane and trifluoroacetate. This-complex [Cu(H2O)( 3)(OOC-CF3) (2)] . 2(C4H8O2) crystallizes in the triclinic space group P1 w ith a= 6.067(1)Angstrom, b = 12.153 Angstrom = 15.057(3)Angstrom, alpha= 10 0.09(2), beta= 99.15(2), gamma= 101.00(2) and Z = 2. The single crystal EPR spectrum of (1) shows to signals (gl = 2.19 and g parallel to = 2.39), and a weak multiplet at g = 4.55. The EPR spectrum of complex (1) is interpret ed as a weak exchange occurring in the chain structure found by X-ray diffr action. A hydrogen bond occurring between the axial water on one copper and the carboxylate group of a neighbor copper is proposed to transmit the mag netic exchange found by EPR. The magnetic susceptibility of (1) gave a cons tant value for the magnetic moment of 1.93 B.M. Bis(1,3-diaminopropan-2-ol)bis(trifluoroacetate)copper(II) complex (2) [Cu( DAP)(2)(OOC-CF3)(2)] (DAP=1,3-diamino propan-2-ol) forms a net of hydrogen bonds in the plane of the DAP ligand with adjacent trifluoroacetates. This complex crystallizes in the monoclinic space group P2(1)/c with a = 9.951(3 )Angstrom, b = 8.521(2) Angstrom, c = 11.224(3)Angstrom, beta= 109.83(2) an d Z = 2. Complex (2) present a weak magnetic coupling; the magnetic data fi ts to the Curie-Weiss equation, with theta= -3.86 K and g = 2.1. The effect ive magnetic moment of (2) decays steadily from 2.01 B.M. at room temperatu re down to 1.5 B.M. at 6 K.